Accelerator Instrumentation RD. Monday, July 14, 2003 Marc Ross

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1 Monday, Marc Ross

2 Linear Collider RD Most RD funds address the most serious cost driver energy The most serious impact of the late technology choice is the failure to adequately address luminosity RD issues 2 Date

3 (not including physics of beams) gradient & RF power & associated diagnostics Low power µwave circuitry Lasers Positioning/alignment/vibration stabilization mm wave & FIR diagnostics Data flow control system Radiation effects Vacuum Feedback Engineering fabrication, packaging, testing Limiting LC technology: energy luminosity 3 Date

4 R&D Challenges 1. Precision microwave 2. IR final doublet girder (~ internal to detector) 3. Beam size from optical transition/diffraction radiation 4. Bunch length 5. Storage ring instabilities electron cloud surface physics 6. Radiation modeling 7. Permanent Magnets 8. RF breakdown 9. Control system From the April 2002 LCRD kickoff meeting 4 Date

5 Cost drivers (%) Warm Inj 15 ML 54 BD 8 Ctrl 4 Other 18 Cold Inj 23* ML 49 BD 8 Ctrl 3 Other 18 ML EDI 14 RF source/dist 40 Girder 18 Civil 18 Other 10 ML EDI 13 Cryo 38 RF 19 Civil 12 Other 16 unofficial, ~personal, estimates 5 Date

6 Risk/cost Drivers (1) Risk can be assessed many ways according to different metrics Example: Availability simulation assessment of risk Cold linac cryomodule The risk is: availability of the cryomodule, especially active components within it All will agree that careful engineering is needed to mitigate risk and make sure that the: Cavity tuners Piezo tuners Coupler interlocks Cold moving parts Are as reliable and as reasonable as possible and that failures are soft 6 Date

7 What happens when... a cryomodule component fails? Availability simulation many cryomodule components are needed for stabilization systems/protection systems first order effect may be negligible... depends on the intrinsic stability depends on the variability of beam parameters how well integrated are the cryo RF controls? (example of TTF, JLAB) 7 Date

8 Risk/cost Drivers (2) Both warm and cold: Linac emittance propagation spurious dispersion is extremely important for both (perhaps single most important effect) impact of BPM performance impact of mis-alignment impact of tuning time Additional beam size instrumentation within the linac is there a need for instrumentation within the cold systems? (not the TDR paradigm) What about the cold BPM s? how reliable are they? 8 Date

9 RD Most emittance dilution begins with a simple linear correlation can catch and correct beam position monitors beam correlation monitors Longitudinal phase space usually involved difficult to image directly Controls/electronics can have large leverage on cost national labs now substantially lag in this technology integration 9 Date

10 Three examples: correlation monitors recent results Multi-bunch behavior of uwave cavity BPM s crude estimates/interesting pathologies longitudinal phase space recent results extremely short bunches/bunch shaping 10Date

11 θ δ/2 σ z Cavity active length Cavity BPM beam Correlation monitor: Deflection cavity/detector BPM I/Q cavity response with deflection cavity at full voltage Axes show directions of pure displacement (black) and pure angle (bluish) (green is 90 from pure displacement) Tilter motion is not quite orthogonal Ellipticity is the ellipse aspect ratio This plot shows equivalent angle trajectory Coupled out to mixer

12 Effective beam tilt scale full width dipole projection is 0.9 of displacement for 8 mm bunch (scales with bunch length) See 29 um peak to peak kick at full I and 20 um projected dipole at monitor Good vertical streak of 7 um beam! Tilt angle 20um/8mm = 2.5 mrad 29um ellipticity Comparison 3.5 and.4 ma 3.5mA 0.4mA 25um 21um dipole 14um dipole

13 Estimate of bunch length from ellipticity Ellipse min/max vs bunch length (mm) for C-band Only length scale used is RF wavelength ATF bunch length range 13Date

14 Summary of bunch length measurements Data file Condition ellipticity bunch length (mm) ATF datac8 nominal I= 3.5mA datac ma datac ma datac ma datac12 0.3mA Vc 150 KV First bunch length measurement made entirely using RF cavities Beam/monitor jitter ~ 1 um (very stable over hours!) 14Date

15 High Bandwidth Cavity BPMs for Multibunch Can imagine building a low Q cavity. Strong coupling difficult Fundamental mode overlap problem increases. Can look at signals from standard cavity BPM with higher bandwidth electronics. Integration time of 3ns vs ~300ns causes a loss of X10 (?) in resolution. Since bunches add coherently, train offsets or tilts can generate very large signals. 15Date

16 1um bunch noise 100nm train offset Simulated Multibunch Signals 1um bunch noise 1um train offset 1um bunch noise 1um train tilt

17 With C-band cavity, 357MHz, Best "conventional" electronics: ~5nm resolution, 1um maximum train offset With 30GHz cavities, resolution ~1nm, but maximum train offset ~200nm

18 Phase space diagnostics based on deflecting/ crab RF Opens up new level of beam control and monitoring active projects at SLAC (SPPS) & DESY (TTF2) Extensive use planned for FEL s, where short bunches critical Needed for finite crossing angle machines big impact on L Needed to correct in addition to diagnose 18Date

19 Krejcik/Emma - LCLS

20 Krejcik/Emma - LCLS

21 Krejcik/Emma - LCLS

22 Krejcik/Emma - LCLS

23 Krejcik/Emma - LCLS

24 HEP must aggressively attack Controls/Instrumentation issues System challenges are clearly greater for HEP machines Look at the shift SLAC.DESY.KEK accelerator groups away from HEP toward nuclear/synchrotron radiation/fel physics and technology very active growth field Many accelerator designers have no intrinsic connection with HEP 24Date